2005
DOI: 10.1143/jpsj.74.3155
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Anomalous Magnetization of Two-Dimensional S = 1/2 Frustrated Square-Lattice Antiferromagnet (CuCl)LaNb2O7

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Cited by 35 publications
(53 citation statements)
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“…The magnetic susceptibility χ of this system, shown in Fig. 2, exhibits typical spin-gap behavior with an estimated gap ∆/k B = 27 K. The spin gap was directly observed by inelastic neutron scattering 11 and high-field magnetization 12 . The very small Weiss temperature Θ = J 1 + J 2 ≤ 5 K in the 1/χ plot ( Fig.…”
Section: Introductionmentioning
confidence: 73%
“…The magnetic susceptibility χ of this system, shown in Fig. 2, exhibits typical spin-gap behavior with an estimated gap ∆/k B = 27 K. The spin gap was directly observed by inelastic neutron scattering 11 and high-field magnetization 12 . The very small Weiss temperature Θ = J 1 + J 2 ≤ 5 K in the 1/χ plot ( Fig.…”
Section: Introductionmentioning
confidence: 73%
“…4 This suggests that, at least within the J -J x -J y model, the ground state should belong to the DS-II region as described in Fig. 3 and there should be substantial state is found for small |J x |,|J y | 0.5J , while the ferromagnetic state stabilizes for larger |J x | and |J y |.…”
Section: Relation To the Experiments On (Cucl)lanb 2 Omentioning
confidence: 88%
“…ðFeClÞLaNb 2 O 7 with S ¼ 2 undergoes a conventional antiferromagnetic order at 78 K, though there is an anomaly in the magnetic susceptibility at around 8 K [5]. An unusual behavior characterized by the spin liquid has been found in an S ¼ 1 2 system ðCuClÞLaNb 2 O 7 , where no long-range magnetic order exists even at 0 K and there is an energy gap of 2.3 meV between the spin-singlet ground state and the first excited triplet state [6,7]. Such a spin-liquid state on the square lattice is interesting in connection with the RVB state predicted by Anderson after the discovery of high T c superconductivity [8].…”
Section: Introductionmentioning
confidence: 99%